1 / 39

ELECTRIC DRIVES

ELECTRIC DRIVES. Ion Boldea S.A.Nasar 1998. 10. SYNCHRONOUS MOTORS FOR DRIVES. 10.1. INTRODUCTION.

dafydd
Download Presentation

ELECTRIC DRIVES

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. ELECTRIC DRIVES Ion Boldea S.A.Nasar 1998 Electric Drives

  2. 10. SYNCHRONOUS MOTORS FOR DRIVES 10.1. INTRODUCTION Synchronous motors (SMs) are in general three phase a.c. fed in the stator and d.c. (or PM) excited in the rotor. As the stator currents produce an m.m.f. traveling at the electric speed w1: (10.1) the rotor m.m.f. (or PM) is fixed to the rotor. The rotor electrical speed wr is: (10.2) in order to obtain two m.m.f. waves at standstill with each other. It is a known fact that only in this situation a non zero average torque per revolution is obtained. Yet, in an alternative interpretation, non zero average torque is produced when the magnetic coenergy in the machine Wco varies with rotor position: (10.3) Electric Drives

  3. 10.2. CONSTRUCTION ASPECTS • As with any electrical motor, the SM has a stator and a rotor. The stator is made of a laminated core with uniform slotting. The stator slots accommodate in general a three phase single or double layer winding made like for induction motors. • In general the number of slots per pole and phase q  2 and thus the coupling inductances vary sinusoidally with rotor position. However in small power PM - SMs concentrated windings may be used (q = 1 slot per pole per phase) when the sinusoidality is lost [1,2]. • On the other hand the SM rotors may be: • active: - excited • - with PMs • passive: - highly anisotropic (variable reluctance) Electric Drives

  4. Figure 10.1 shows salient pole SMs with excited and PM rotors while figure 10.2 exhibits nonsalient pole SMs. Figure 10.1. Salient pole active rotor SMs with a.) excited rotor b.) interior PMs Electric Drives

  5. Figure 10.2. Nonsalient pole active rotors of SMs a.) excited b.) with surface PM Electric Drives

  6. Figure 10.3. Passive - anisotropic (reluctance) - rotors for SMs a.) multiple flux barrier rotor b.) axially - laminated - anisotropic (ALA) rotor Electric Drives

  7. 10.3. PULSATING TORQUE • It is a known fact that an ideal SM - with sinusoidal m.m.f. and constant airgap - when fed with sinusoidal symmetric currents in the stator at frequency w1 = wr (wr - rotor speed) - produces a constant torque. • In reality pulsating torques may occur due to: • a. stator (and rotor) slot openings; • b. magnetic saturation caused flux harmonics; • c. current waveforms; • d. PM field pulsations due to stator slot openings (cogging torque). • Items a to c cause the so called electromagnetic pulsating torques while d causes the zero stator current or cogging torque. • Rotor pole (or PM) span correlation with stator slot openings, stator slot inclination or PM pole inclination, fractional q (slots per pole and phase) and, finally, special current waveform shaping through PEC control are all methods to reduce these, basically reluctance, parasitic torques [4] to less than 1% of rated torques. High performance smooth torque drives capable to operate below 20rpm in sensorless control or under 1rpm with position sensor control are thus obtained. Electric Drives

  8. 10.4. THE PHASE COORDINATE MODEL The phase coordinate model is based on phase equations using stator and rotor circuits. For q  2 (slots per pole per phase) - distributed windings - the inductance matrix contains sinusoidal terms. We will take the case of salient pole rotor as the nonsalient pole rotor is a particular case of the former. The phase inductance matrix [L] is (see figure 10.1 and 10.2): (10.4) Electric Drives

  9. For distributed windings (q  2) all the stator self and mutual and stator - rotor inductances are rotor position, qer, dependent: (10.5) Electric Drives

  10. On the other hand, for concentrated windings (q = 1), when nonsalient pole PM rotors are used, all stator inductances are independent of rotor position, the rotor cage is eliminated. Only the motion - related inductances between the constant field - current PM equivalent circuit and the stator windings depend on rotor position. (10.7) The voltage - current matrix equation in phase coordinates (stator coordinates for stator, rotor coordinates for rotor) are: (10.8) with (10.9) (10.10) Electric Drives

  11. (10.11) (10.12) Finally the electromagnetic torque Te may be calculated from the coenergy derivative with respect to rotor position: (10.13) After neglecting magnetic saturation, we multiply equation (10.8) by : (10.14) The last term is the electromagnetic power Pelm: (10.15) The motion equations are: (10.16) Electric Drives

  12. 10.5. THE SPACE PHASOR (d-q) MODEL Proceeding as for the induction motor we may define the stator current space phasor, in stator coordinates: (10.17) On the other hand, from (10.9) with (10.4), the phase a flux linkage la is: (10.18) Making use of the inductance definition of (10.5) we find: (10.19) The stator flux space phasor is: (10.20) Making use of (10.18) for lb, lc, (10.20) yields: (10.21) Electric Drives

  13. Multiplying (10.21) by we obtain: (10.22) We should now notice that: (10.23) are space phasors in rotor coordinates (aligned with rotor d axis). With (10.23), (10.22) becomes: (10.24) Next, the stator phase equations in stator coordinates are: (10.25) Electric Drives

  14. We may translate them in space phasors as: (10.26) The final form of (10.26) is: (10.27) and (10.28) Equation (10.27) is, in fact, identical to that for the induction machine. Only the flux expression (10.24) is different. (10.29) (10.30) with (10.31) Electric Drives

  15. We may reduce the rotor to stator currents: (10.32) (10.33) Magnetic saturation may be accounted by unique ldm(im) and lqm(im) functions to be either calculated or measured [5]. The stator equation (10.27) in d - q coordinates becomes: (10.34) (10.35) Now we should add the rotor equations in rotor d - q coordinates (as along axis d and q the rotor windings are not at all symmetric): (10.36) Electric Drives

  16. (10.37) (10.38) The torque, Te, is: (10.39) Finally the d - q variables are related to the abc variables by the Park transformation: (10.40) Electric Drives

  17. Electric Drives

  18. Figure 10.4. Signal flow diagram of SMs Electric Drives

  19. PM or reluctance rotor SMs used for variable speed lack the excitation winding and if = const (zero for RSM). They also lack the damper cage (tdr = trd’ = tqr = tqr’ = 0) (figure 10.5). Electric Drives

  20. Figure 10.5. Flow signal diagram of PM and reluctance SMs (no rotor damper cage) Figure 10.6. SM equivalent circuits Electric Drives

  21. 10.6. STEADY STATE OPERATION For steady state the stator phase voltages are given by: (10.44) where w1 = const., and thus the rotor position qer is: (10.45) Notice that wr = wr0 = w1 for steady state. Using (10.40) the d - q voltage components Vd, Vq in rotor coordinates are: (10.46) As Vd, Vq are time independent so will be the currents in the stator: id, iq. Also d/dt = 0 (s = 0) and thus from (10.38) (zero damper cage currents) and if = if0 = Vf / rf = const. Electric Drives

  22. The space phasor diagram follows from equations ((10.34) - (10.35)) which may be written in space phasor form as the stator is symmetric electrically and magnetically (figure 10.7). (10.47) For steady state all variables in the space phasor (or d - q) model are d.c. quantities. Space angles translate into time phase shift angles between stator quantities (like j1 - the power factor angle) in phase coordinates. Figure 10.7. SM - steady state - with excitation or PMs a.) d - q axis model b.) space phasor diagram Using the d - q model for speed control is thus ideal as steady state means d.c. Electric Drives

  23. 10.7. TO VARY SPEED VARIABLE FREQUENCY IS MANDATORY • SMs keep a tight relationship between speed and frequency as the rotor m.m.f. (if any) is of d.c. (or PM) character: • (10.48) • Varying the number of pole pairs p is unusual so, in fact, to vary speed variable frequency is mandatory. • Example 10.1. Unity power factor and constant stator flux. • Let us consider an excited synchronous motor with the data: Vn = 600V (line voltage, rms, star connection), In = 500/ (rms), rs = 0.016W, Ld = 2Lq = 0.0056H, Lsl = 0.1Ld, w1 = 2p60rad/s, p = 2 pole pairs. • Determine: • The steady state space phasor diagram for unity power factor (j1 = 0) • Calculate the values of if, id, iq for unity power factor and rated phase current, In. • Calculate the torque for j1 = 0. • Derive and plot the torque - speed curve for rated and half rated stator flux for variable frequency and constant stator voltage. Electric Drives

  24. Solution: a. The required space phasor diagram comes from figure 10.7.b with j1=0. Figure 10.8. Space phasor diagram for unity power factor • b. From figure 10.8. we have: • (10.49) • (10.50) Electric Drives

  25. For no load (10.51) (10.52) From (10.49) the rated stator flux ls is: (10.53) (10.54) (10.55) Thus (10.56) (10.57) (10.58) Electric Drives

  26. (10.59) (10.60) The field current if (reduced to the stator) is: (10.61) The electromagnetic torque Te is: (10.62) Notice that for cosj1 = 1 the torque expression (10.39) may be written as: (10.63) The stator flux and current space phasors are rectangular, like in a d.c. motor. Consequently for constant stator flux ls the torque is proportional to stator current. Varying the frequency w1 = wr, such that ls = const and cosj1 = 1 appears as an optimum way to speed control. Electric Drives

  27. The torque - speed curve may be derived from (10.49) with (10.63) by eliminating the stator current is: (10.64) (10.65) As w1 = wr, varying speed means, implicitly, that the frequency changes. The torque - speed curve is a straight line like in a separately excited d.c. brush motor. The ideal no load speed (Te = 0) wr0 is: (10.66) For rated flux and full voltage, Vsn, the base speed wb is obtained. Above the base speed wr0 may be modified only through flux weakening like in a d.c. brush motor. Halving the flux doubles the ideal no load speed wr0. The torque speed curves are illustrated on figure 10.9. Electric Drives

  28. Figure 10.9. Speed - torque curves for constant flux and unity power factor Four quadrant operation is implicit as negative frequency w1 = wr means negative order (a c  b instead of a  b  c) of stator phases fed from a PEC. Electric Drives

  29. Example 10.3. PM - SM, operation for constant id. • A nonsalient pole rotor PM - SM has the data: Vn = 180V (rms, line voltage), Ld = 0.4Lq = 0.05H rs = 1W, no load line voltage (rms) at nn = 1500rpm (f1 = 60Hz), Von = 180V (rms). • Determine: • The PM flux linkage lPM; • The torque - speed curve for id = 0, id = 5A and the ideal no load speed in the three cases, stator flux and torque for iq = 10A; • Draw d - q equivalent circuits for steady state and introduce the iron losses in the model. • Solution: • The no load voltage Von “translated” into space - vector terms, Vs0: • (10.80) • According to (10.50): • (10.81) • (10.82) Electric Drives

  30. (10.83) (10.84) As (10.85) The electromagnetic torque Te is: (10.86) The d - q voltage components ((10.34) - (10.35)), with d/dt = 0, are: (10.87) Now we replace iq from (10.86) into (10.87). Thus we have: (10.88) Electric Drives

  31. or (10.89) The ideal no load (Te = 0) speed wr0 is: (10.90) For id = 0: (10.91) Also: (10.92) (10.93) Electric Drives

  32. Notice that id < 0 means a demagnetising effect. However the torque expression (10.86) shows that as Ld < Lq only id < 0 produces a positive torque contribution. A positive torque contribution for id < 0 is accompanied by a reduction in the stator flux as: (10.94) (10.95) The torque for id = 0, -5A, +5A, iq = 10A is: (10.96) (10.97) (10.98) Electric Drives

  33. Though the core losses are related to the main flux components we may assume them to be produced by the stator flux. Figure 10.11. Steady state d - q equivalent circuits of PM - SM with core losses included Electric Drives

  34. Example 10.4. The reluctance synchronous motor (RSM) steady state. • A high performance RSM has the data: Ld = 10Lq = 0.1H, p = 2, rs = 1W, f1 = 60Hz. • Determine: • a.The space - phasor diagram; • b.The maximum torque per given stator current and for given stator flux; • c.Introduce a PM along axis q to reduce the q axis flux. Draw the new space phasor diagram and discuss it. • Calculate the torque for id = 3A, iq = 15A without and with PM flux lPM = -Lqiq. • d. Calculate the stator flux to produce the respective torques. • Solution: • The space phasor diagram is obtained simply from the general one (figure 10.7) with if = 0 and Ld >> Lq (figure 10.12). Electric Drives

  35. Figure 10.12. RSM - space phasor diagram The torque expression (10.86) with if = 0 and Ld >> Lq is: (10.99) The voltage equations (10.87) become: (10.100) Electric Drives

  36. The stator flux and stator current are: (10.101) (10.102) The maximum torque for given stator current, is : (10.103) may be obtained from (10.99) and (10.103): (10.104) After eliminating iq we get: (10.105) If is = in (rated current) the machine is driven into heavy saturation as idi is too high in comparison with the rated no load phase current , with the exception of very low power motors when i0 / in > 0.707. Though it leads to maximum torque per ampere it may be used for torques lower than (50 - 60)% of rated torque. This may be the case for low speed operation in some variable speed drive applications. Electric Drives

  37. On the other hand, for given stator flux (10.101), the maximum torque is obtained for: (10.106) The maximum torque is: (10.107) This time the d - q flux angle d = 450 in figure 10.12. As it provides maximum torque per given flux, this is the limit condition at high speeds when the flux is limited (flux weakening zone). Introducing the PM in axis q: (10.108) In (10.108) to avoid PM demagnetisation. The torque expression (10.86) becomes: (10.109) Electric Drives

  38. Figure 10.13. PM - SRM - space phasor diagram Notice that for motoring d < 0 (the flux vector is lagging (not leading) the d axis) and the power factor has been increased together with torque. Only low remnant flux density (moderate cost) PMs are required as Lqisn is still a small flux (Ld / Lq >> 1). Electric Drives

  39. Let us now calculate the torque and stator flux for the two situations: (10.110) (10.111) (10.112) (10.113) So the PMs in axis q produce almost 10% torque increase for a 10% decrease in flux level. The improvements are more spectacular in lower saliency machines (Ld / Lq = 5 - 8), which are easier to build. Electric Drives

More Related